Matches in SemOpenAlex for { <https://semopenalex.org/work/W2591655608> ?p ?o ?g. }
- W2591655608 abstract "We present numerical results from three-dimensional evolutions of scalar perturbations of Kerr black holes. Our simulations make use of a high-order accurate multiblock code which naturally allows for adapted grids and smooth inner (excision) and outer boundaries. We focus on the quasinormal ringing phase, presenting a systematic method for extraction of the quasinormal mode frequencies and amplitudes and comparing our results against perturbation theory. The detection of a single mode in a ringdown waveform allows for a measurement of the mass and spin of a black hole; a multimode detection would allow a test of the Kerr nature of the source. Since the possibility of a multimode detection depends on the relative mode amplitude, we study this topic in some detail. The amplitude of each mode depends exponentially on the starting time of the quasinormal regime, which is not defined unambiguously. We show that this time-shift problem can be circumvented by looking at appropriately chosen relative mode amplitudes. From our simulations we extract the quasinormal frequencies and the relative and absolute amplitudes of corotating and counterrotating modes (including overtones in the corotating case). We study the dependence of these amplitudes on the shape of the initial perturbation, the angular dependence of the mode, and the black hole spin, comparing against results from perturbation theory in the so-called asymptotic approximation. We also compare the quasinormal frequencies from our numerical simulations with predictions from perturbation theory, finding excellent agreement. For rapidly rotating black holes (of spin $j=0.98$) we can extract the quasinormal frequencies of not only the fundamental mode, but also of the first two overtones. Finally we study under what conditions the relative amplitude between given pairs of modes gets maximally excited and present a quantitative analysis of rotational mode-mode coupling. The main conclusions and techniques of our analysis are quite general and, as such, should be of interest in the study of ringdown gravitational waves produced by astrophysical gravitational wave sources." @default.
- W2591655608 created "2017-03-16" @default.
- W2591655608 creator A5042701304 @default.
- W2591655608 creator A5062835021 @default.
- W2591655608 creator A5073182123 @default.
- W2591655608 creator A5077620063 @default.
- W2591655608 creator A5091293746 @default.
- W2591655608 date "2006-10-24" @default.
- W2591655608 modified "2023-10-18" @default.
- W2591655608 title "Numerical study of the quasinormal mode excitation of Kerr black holes" @default.
- W2591655608 cites W1968369949 @default.
- W2591655608 cites W1984180949 @default.
- W2591655608 cites W1995217152 @default.
- W2591655608 cites W1998021253 @default.
- W2591655608 cites W2003324018 @default.
- W2591655608 cites W2016405928 @default.
- W2591655608 cites W2031486433 @default.
- W2591655608 cites W2040155109 @default.
- W2591655608 cites W2055524364 @default.
- W2591655608 cites W2056723718 @default.
- W2591655608 cites W2069764580 @default.
- W2591655608 cites W2081612620 @default.
- W2591655608 cites W2098703976 @default.
- W2591655608 cites W2104443781 @default.
- W2591655608 cites W2118909459 @default.
- W2591655608 cites W2128918391 @default.
- W2591655608 cites W2134572535 @default.
- W2591655608 cites W2140973976 @default.
- W2591655608 cites W2147829712 @default.
- W2591655608 cites W2150567191 @default.
- W2591655608 cites W2163612506 @default.
- W2591655608 cites W2764789329 @default.
- W2591655608 cites W3103158278 @default.
- W2591655608 cites W3103204141 @default.
- W2591655608 cites W3105039587 @default.
- W2591655608 cites W3105816330 @default.
- W2591655608 cites W4237292901 @default.
- W2591655608 doi "https://doi.org/10.1103/physrevd.74.084028" @default.
- W2591655608 hasPublicationYear "2006" @default.
- W2591655608 type Work @default.
- W2591655608 sameAs 2591655608 @default.
- W2591655608 citedByCount "55" @default.
- W2591655608 countsByYear W25916556082012 @default.
- W2591655608 countsByYear W25916556082013 @default.
- W2591655608 countsByYear W25916556082014 @default.
- W2591655608 countsByYear W25916556082015 @default.
- W2591655608 countsByYear W25916556082017 @default.
- W2591655608 countsByYear W25916556082018 @default.
- W2591655608 countsByYear W25916556082019 @default.
- W2591655608 countsByYear W25916556082020 @default.
- W2591655608 countsByYear W25916556082021 @default.
- W2591655608 countsByYear W25916556082022 @default.
- W2591655608 countsByYear W25916556082023 @default.
- W2591655608 crossrefType "journal-article" @default.
- W2591655608 hasAuthorship W2591655608A5042701304 @default.
- W2591655608 hasAuthorship W2591655608A5062835021 @default.
- W2591655608 hasAuthorship W2591655608A5073182123 @default.
- W2591655608 hasAuthorship W2591655608A5077620063 @default.
- W2591655608 hasAuthorship W2591655608A5091293746 @default.
- W2591655608 hasBestOaLocation W25916556082 @default.
- W2591655608 hasConcept C104954878 @default.
- W2591655608 hasConcept C110521144 @default.
- W2591655608 hasConcept C121332964 @default.
- W2591655608 hasConcept C174256460 @default.
- W2591655608 hasConcept C177918212 @default.
- W2591655608 hasConcept C180205008 @default.
- W2591655608 hasConcept C198394728 @default.
- W2591655608 hasConcept C2524010 @default.
- W2591655608 hasConcept C2780870619 @default.
- W2591655608 hasConcept C30475298 @default.
- W2591655608 hasConcept C3079626 @default.
- W2591655608 hasConcept C31258907 @default.
- W2591655608 hasConcept C32758168 @default.
- W2591655608 hasConcept C33923547 @default.
- W2591655608 hasConcept C41008148 @default.
- W2591655608 hasConcept C50341732 @default.
- W2591655608 hasConcept C57691317 @default.
- W2591655608 hasConcept C62520636 @default.
- W2591655608 hasConcept C74172769 @default.
- W2591655608 hasConcept C74650414 @default.
- W2591655608 hasConcept C88030215 @default.
- W2591655608 hasConcept C89305328 @default.
- W2591655608 hasConceptScore W2591655608C104954878 @default.
- W2591655608 hasConceptScore W2591655608C110521144 @default.
- W2591655608 hasConceptScore W2591655608C121332964 @default.
- W2591655608 hasConceptScore W2591655608C174256460 @default.
- W2591655608 hasConceptScore W2591655608C177918212 @default.
- W2591655608 hasConceptScore W2591655608C180205008 @default.
- W2591655608 hasConceptScore W2591655608C198394728 @default.
- W2591655608 hasConceptScore W2591655608C2524010 @default.
- W2591655608 hasConceptScore W2591655608C2780870619 @default.
- W2591655608 hasConceptScore W2591655608C30475298 @default.
- W2591655608 hasConceptScore W2591655608C3079626 @default.
- W2591655608 hasConceptScore W2591655608C31258907 @default.
- W2591655608 hasConceptScore W2591655608C32758168 @default.
- W2591655608 hasConceptScore W2591655608C33923547 @default.
- W2591655608 hasConceptScore W2591655608C41008148 @default.
- W2591655608 hasConceptScore W2591655608C50341732 @default.
- W2591655608 hasConceptScore W2591655608C57691317 @default.
- W2591655608 hasConceptScore W2591655608C62520636 @default.